OBJECT OF THE INVENTION
[0001] The present invention, as expressed in that stated in this descriptive report, refers
to a process for obtaining spectral voids in the transmission of signals over the
electric network. A spectral void is defined as a frequency band in which the density
of power transmitted is less than the certain value required. This process is specially
important in the creation and use of the transmission system over the electric network,
as it permits the power of the signal transmitted to be adjusted to different frequencies
so that it can adjust to the regulations established by the current rules in different
countries for the transmission of signals over the electric network, with the adequate
spectral voids specified by these rules. In this way, interference with licensed services
that use the same frequency band as the signal transmitted by the communications over
the electric network will be avoided.
BACKGROUND TO THE INVENTION
[0002] The means of communication constituted by the electric network, both low and medium
voltage, is a means that was not initially conceived for the transmission of telecommunications
signals. This means is an unscreened means in which the signal transmitted can radiate
and interfere with other systems that are using the same frequencies. The case of
amateur radio enthusiasts and other radio-communications services that include radio
navigation, emergency services, etc. are relevant. In these services, a low interfering
signal can interrupt the communication, for which reason it is particularly important
to avoid power transmission at these frequencies.
[0003] It is because of this that the rules in force in many countries impose restrictions
on power spectral density (PSD) that can be transmitted on certain frequencies, so
that it is necessary to obtain deep spectral voids for transmitting signals over the
electric network according to the rules. The process that is the object of the invention
is designed to create spectral voids of great depth with the maximum efficiency possible,
covering the bandwidth strictly necessary.
[0004] This process seeks the adjustment of the signal transmitted to certain patterns of
power imposed by the aforementioned legal reasons in an efficient manner. These power
patterns tend to be defined as frequency ranges in which power transmission is strictly
limited (for example, 30 dB less with respect to other frequencies) or even prohibited.
Nevertheless, given the technological limitations it is not possible to obtain immediate
transition between a frequency band with a particular power spectral density and another
one with a different power spectral density, so it is not possible to abruptly eliminate
the signal transmitted in a certain frequency range without reducing the power of
the adjacent carriers to the spectral void. Thanks to the invention process this reduction
can be performed in an efficient manner, by reducing the number of carriers adjacent
to the spectral void affected by generating this spectral void to the maximum.
[0006] The new aspect of the invention process lies in producing spectral voids of more
than 30 dB in a band in an efficient manner, by means of adjusting the power sent
in certain carriers, the windowing of OFDM symbols plus the cyclic prefix and the
use of suitable values for the number of active carriers and the size of the IDFT;
something that cannot be deduced from the previous state of the art of this patent.
DESCRIPTION OF THE INVENTION
[0007] In order to achieve the objectives and prevent the inconveniences indicated in previous
sections, the invention consists of a process for obtaining spectral voids in the
transmission of signals over the electric network that includes sending signals by
means of orthogonal frequency division multiplexing (OFDM), where the communication
nodes have a transmitter, means for adding a cyclic prefix and means for converting
frequency to time of OFDM symbols.
[0008] This process is characterised by the fact that it adjusts the power of one or more
OFDM signal carriers selectively by means of attenuation or by the elimination of
these carriers, because it applies the inverse discreet Fourier transform (IDFT) that
is used to transform the signal for frequency domain to the time domain signal with
a number of points that can be selectively greater than or equal to 1024 if the IDFT
is complex or greater than or equal to 2048 if the IDFT is real, and because, once
the cyclic prefix has been added, the OFDM symbols in the time domain are multiplied
by a window. Thanks to this, it is possible to achieve abrupt spectral voids of 20
dB in depth, which is a great advantage since it possible for the signal transmitted
not to interfere with other licensed services that use the same frequency bands as
the signal that is to be transmitted over the electric network. In the same way, the
invention process permits the power spectral density selected for transmitting the
signal to be adjusted, thanks to the possibility of introducing spectral voids in
the band.
[0009] In the execution of the invention, the window used is a risen cosine window. This
window was selected for having a flat area in time and due to its spectral characteristics.
[0010] In another execution of the invention, this risen cosine window, which can be defined
from the rolloff factor, has a rolloff factor of less than or equal to 0.2.
[0011] Furthermore, the window has a size in the number of samples that is greater than
or equal to 2048, where these samples are digital samples previous to the digital
analogue converter (DAC) of the transmitter.
[0012] On the other hand, the number of carriers whose power is adjusted depends on the
situation, width and depth of the spectral voids and the form of the window selected
for the process. To produce a spectral void of suitable depth, the power of the carriers
located in the spectral void and the number of carriers adjacent to the previous ones
are adjusted. The faster the secondary lobes in the frequency representation in the
window selected roll off, the fewer the number of the adjacent carriers that have
to be adjusted for reaching the width and depth of the spectral void required. To
make power adjustments to the suitable carriers, various processes can be used that
can be combined. The adjustment can be made through gradual attenuation, so that the
main lobe of the signal transmitted in the carriers in the spectral void, or the secondary
lobes of the signals transmitted if the said carriers are adjacent, whether less than
the power spectral density required for the signal transmitted.
[0013] Another way of performing the adjustment is the direct elimination of the carriers
affected, this elimination referring to not transmitting any power in the carriers
to be adjusted, in such a way that the carriers located in the spectral void are eliminated
together with a number of adjacent carriers suitable for ensuring that the power spectral
density is less than that required for the signal transmitted in the spectral void.
[0014] The two adjustment processes can be used independently in the carriers necessary
or can be combined, being able to eliminate certain carriers and attenuate others.
[0015] In order to facilitate best understanding of this descriptive report and forming
an integral part of it, some figures are included below in which the object of the
invention is shown as an illustration and not limiting in any way.
BRIEF DESCRIPTION OF THE FIGURES
[0016]
Figure 1.- This shows an example of power spectral density (PSD) that the rules require for
the transmission of signals on the 2 to 30 dB bandwidth for protecting services licensed
on these frequencies.
Figure 2.- This shows an example of a window that can be used in the invention process.
Figure 3.- This shows a block diagram of the windowing process of a sampled signal.
Figure 4.- This shows various typical windows both in time and in frequency.
Figure 5.- This shows risen cosine windows with various rolloff factors (β) both in time and
in frequency.
Figure 6- This shows a block diagram of the process for creating spectral voids in transmission.
Figure 7- This shows the windows used in the example for achieving a 30 dB deep spectral void.
DESCRIPTION OF AN EMBODIMENT OF THE INVENTION
[0017] A description is given below of an example of the invention, making reference to
the numbering adopted in the figures.
[0018] In the transmission of signals and the design of communications systems over the
electric network, one of the most important problems is that the transmission means
is not screened and part of the signal transmitted to the electric network is transmitted
to the exterior, being able to interfere with licensed systems that use a range of
frequencies overlapped by the range of frequencies used in the signal transmitted.
[0019] With the object of reducing this interference, many countries have rules on the maximum
power spectral density that can be transmitted or introduced in the electricity line.
Unfortunately, these rules vary from one country to another and therefore it is necessary
to create abrupt spectral voids in the spectrum that can be adjusted to prevent transmitting
on certain frequencies depending on the country. An example can be seen in figure
1 of the power spectral density that will be required to be able to transmit signals
between 2 and 30 MHz. As can be observed, multiple spectral voids exist that have
to be respected in order to transmit on this bandwidth.
[0020] The invention process allows the creation of these spectral voids in the signal transmitted
in an efficient manner and, therefore, adjust to the adequate spectral density in
any case.
[0021] As explained previously, the invention process uses the windowing concept, which
is known in the state of the art. Unfortunately, depending on the technical source
chosen this concept can be interpreted in one way or another, for which reason before
including an example of the execution of the invention process, the "window" definition
criterion used in this process will be stated.
[0022] Windowing a digital signal consists of multiplying the samples of a signal by a window.
This window is another digital signal that, in general, has a set of adjacent samples
different from cero. An example of a window centred on sample 0 can be seen in figure
2.
[0023] Once the window to be used in the process has been chosen, it is necessary to carry
out the windowing. The signal windowing process can be seen in figure 3. This windowing
is performed by means of multiplying (1) the signal samples by the window samples
(for which the window has to move to the appropriate position, instead of sample 0).
The signal windowing process (multiplication of the time domain) affects the signal
in the frequency domain. This dependence can be observed in the modulation or windowing
theorem:

[0024] This theorem shows that multiplication in the time domain produces a periodic convolution
of the shape of the window in the frequency domain. The secondary lobes of the window
in the frequency domain will determine the frequency form of the y[n] output signal.
The shape in the time and frequency domain of some typical windows (triangular, Bartlett
and Chebyshev) known in the state of the art can be observed in figure 4. In this
figure it can be seen that the shape of the window determines the secondary lobes
of the frequency response. For example, the Chebyshev frequency response is maintained
constant (in the secondary lobes), while for Bartlett it is higher in the initial
secondary lobes but falls very rapidly in the following ones.
[0025] For the execution example described, the preferred window is a risen cosine window.
The formula of the risen cosine window centred on sample cero is shown below:

[0026] Where N is the size of the window defined as the values of the window with value
(v[n]) above 0.5, and β being the rolloff factor. In general, a risen cosine window
can be defined by this rolloff factor β. This factor will always be between 0 and
1 and indicates the excess signal transmitted. The higher the rolloff factor, the
more gentle the rolloff, as can be observed in figure 5. Several risen cosine windows
both in time and frequency and their dependency on the rolloff factor (β) are shown
in this figure. When the rolloff factor reaches 0, the window becomes a rectangular
window that presents secondary lobes with very high frequency.
[0027] If the rolloff value is increased, less elevated secondary lobes are achieved in
exchange for sacrificing efficiency. This loss of efficiency is due to the fact that
the window increases in size (where the excess is calculated as being N*β). On the
other hand, if a rolloff factor that is too low is used, efficiency is lost because
the secondary lobes do not drop sufficiently and, in this case, it becomes necessary
to increase the number of carriers adjacent to the spectral voids that have be adjusted
in power.
[0028] A way of increasing efficiency while maintaining the rolloff factor is to increase
the number of carriers of the OFDM signal. The number of adjacent carriers that have
to adjust to create a spectral void will not vary with regard to the previous case
but, since the total number of carriers is greater, the loss in efficiency will be
lower in percentage. For this reason, the process becomes applicable from a specific
number of IDFT carriers onwards.
[0029] when preparing a design for the transmission of signals over the electric network,
it has been calculated that the rolloff factor has to be less than 0.2 in order to
have high efficiency. In the same way, the number of samples of the window must be
greater than 2048. For this specific example of execution of the invention, a 0.15
rolloff factor, a 0.05 factor and 2600 samples will be used.
[0030] To carry out the invention process on the signal being transmitted (once the window
has been chosen), a block diagram like the one shown in figure 6 is used. In this
figure, the signal to be transmitted is entered in each OFDM signal carrier in a block
(2) that adjusts the power of the appropriate carriers to create the necessary spectral
voids. Carriers located in the spectral void together with their adjacent carriers
will mainly be adjusted. The greater the rolloff of the secondary lobes in the risen
cosine window chosen, the lower the number of adjacent carriers will have to be affected
to achieve the spectral void. Afterwards, block (3) in this example of execution carries
out the inverse fast Fourier transform (IFFT) in a complex manner that is usually
used to implement the inverse discrete Fourier transform (IDFT) with OFDM modulations.
Following this, block (4) inserts the cyclic prefix generated by block (5) and block
(6) multiplies the digital signal of the time domain by the window generated by block
(7). For the spectral void generation process to be efficient it is necessary to use
an OFDM with multiple carriers and IFFT with a great number of points. In this example
of execution, a complex 1024-point IFFT is used.
[0031] Finally, before transmitting and although this block does not appear in figure 6,
the digital signal will be converted to an analogue one by means of the DAC converter.
[0032] To achieve abrupt spectral voids the attenuation or elimination of the carriers located
in the frequency positions within the spectral void is not sufficient. This is due
to the fact that there is power remaining due to the secondary lobes of the adjacent
carriers which is produced, to a large extent, due to the transitions of the OFDM
signal that reach the spectral area where the spectral void should be. To avoid this
it is necessary to adjust the power or to also eliminate a certain number of carriers
adjacent to the carriers located in the positions at the ends of the spectral void.
This is dealt with by block (2) in figure 6. Depending on the shape of the risen cosine
window generated by block (7), the number of adjacent carriers whose power has to
be modified will be greater or lesser, for which reason both blocks are inter-related.
[0033] The shape of two risen cosine windows with the values chosen in this execution example
(rolloff factor 0.15 and rolloff factor 0.05, and number of samples 2600) can be seen
in figure 7. In this case, for example, if a 30 dB deep spectral void is to be achieved,
the power of 4 adjacent carriers would have to be adjusted in the case of using the
invention process with one risen cosine window with a rolloff factor of 0.15 and a
total of 7 adjacent carriers in the case of using a rolloff factor of 0.05.
1. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, that includes sending signals by means of orthogonal frequency division multiplexing
(OFDM), where communication nodes have a transmitter, means for adding a cyclic prefix
and means for converting the frequency of OFDM symbols to time; wherein this includes:
- adjusting power of one or more OFDM signal carriers by means of a process selected
from attenuation and elimination of these carriers;
- applying a inverse discreet Fourier transform (IDFT) that is used to transform the
signal for frequency domain to time domain signal with a number of points of at least
1024 if said IDFT is complex, and of at least 2048 if the IDFT is real;
- adding a cyclic prefix, and then multiplying the OFDM symbols in the time domain
by a window;
to achieve an effect selected from achieving abrupt spectral voids of over 30 dB in
depth and without interfering with other licensed services that use the same frequency
bands, achieving compliance with the power spectral density required for transmitting
the signal and a combination thereof.
2. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, according to claim 1, wherein the window used to obtain the abrupt spectral voids
is a risen cosine window.
3. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, according to claim 2, wherein the risen cosine window has a maximum rolloff factor
of 0.2.
4. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, according to claim 1, wherein the window has a number of samples of at least 2048,
where said samples are digital samples previous to a digital analogue converter (DAC)
of the transmitter.
5. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, according to claim 1, wherein the number of carriers whose power is adjusted depends
on the position, width and depth of the spectral voids, and on a shape of the window,
so therefore to produce a spectral void the power of the carriers located in that
spectral void is adjusted as well as the power of the carriers adjacent to the formers,
which will be lower the faster the secondary lobes of the window used for the transmission
process decrease.
6. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, according to claim 1, wherein the adjustment of the power of the carriers is made
by means of gradual attenuation, for the lobe selected from the main lobe of the signal
transmitted in the carriers within the spectral void and the secondary lobes of the
signals transmitted if these carriers are adjacent, to be less than the power spectral
density (PSD) demanded for the signal transmitted in the spectral void.
7. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, according to claim 1, wherein the adjustment of the power of the carriers is made
by means of the elimination of carriers, this elimination referring to not transmitting
any power in the carrier to be adjusted, to eliminate the carriers located within
the spectral void and a sufficient number of adjacent carriers to achieve that the
power spectral density (PSD) is less than that required for the signal transmitted
in the spectral void.
8. METHOD OF OBTAINING SPECTRAL VOIDS IN THE TRANSMISSION OF SIGNALS OVER THE ELECTRIC
NETWORK, according to any of claims 6 and 7, wherein the adjustment of the carriers is accomplished
by means of a process selected from gradual attenuation, elimination and combination
thereof.